Published August 2017 | Version v1
Journal article

Deposition of carbon inside gaps of castellated tungsten blocks with intrinsic misalignment

  • 1. National Fusion Research Institute, Daejeon (Korea, Republic of)
  • 2. Department of electrical engineering, Hanyang University, Seoul (Korea, Republic of)

Description

Highlight• The castellated blocks are manufactured and installed at central divertor in KSTAR. • The surface density of inside the toroidal and poloidal gap of castellated blocks is in a range from 0.5×1015 up to 6.7×1015 atom/cm2. • Compare the carbon deposition on the toroidal and poloidal gaps, contribution of each species can be separated. • The contribution of neutrals is common for both gaps. • The carbon density on chamfered shape is the lowest in to the four shapes. • At the Raman spectra, decrease of I(D)/I(G) as a function of distance from the gap entrance indicates the increase of hydrogen contents. When PFCs have castellated structure, co-deposition of fuel inside gaps between castellated blocks is an important issue. Four different shapes of castellated tungsten blocks were fabricated to study corresponding issues in KSTAR: Conventional "basic" rectangular shape, single chamfer leading edge, double-chamfer and rounded edge, with two different poloidal gap distances of 0.5 mm and 1.0 mm. These tungsten blocks were exposed plasma of L- and H-mode discharges during a whole campaign in 2014. The blocks were taken out from the vacuum vessel after the campaign. Gap deposition was analyzed by Electron Probe X-ray Micro Analyzer (EPMA) to obtain carbon surface density (atoms/cm2), and by Raman spectroscopy to identify chemical bonding structure of carbon deposits in gaps. The carbon surface density in toroidal and poloidal gaps was in a range from 0.5 × 1015 atom/cm2 up to 6.7 × 1015 atom/cm2. At the gap entrance, contribution of ions is 6.0–6.7 × 1015 atom/cm2, decreased down to 1.0 × 1015 atom/cm2 at a depth of 0.5 mm, and remains constant afterwards. The contribution of charge exchange neutral is about 3.0 × 1015 atom/cm2 at the gap entrance, and then gradually decreases as a function of distance from the entrance. Deposition in 1.0 mm wide gaps show much larger deposition patterns and that particles have reached much deeper inside the gap. Raman spectra show that the intensity ratio I(D)/I(G) decreases from top to the depth of 5 mm indicating the increase of hydrogen contents.

Availability note (English)

Available from http://dx.doi.org/10.1016/j.nme.2017.05.014

Additional details

Identifiers

DOI
10.1016/j.nme.2017.05.014;
PII
S2352179116301351;

Publishing Information

Journal Title
Nuclear Materials and Energy
Journal Volume
12
Journal Page Range
p. 662-667
ISSN
2352-1791

Conference

Title
22. International Conference on Plasma-Surface Interactions in Controlled Fusion Devices
Acronym
PSI-22
Dates
30 May - 3 Jun 2016
Place
Rome (Italy)

Optional Information

Notes
© 2017 The Authors. Published by Elsevier Ltd.